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FormoSat-3 / ROCSat-3 / COSMIC
The ROCSat-3/COSMIC (Republic of
China Satellite-3 / Constellation Observing System for Meteorology,
Ionosphere
and Climate) is an international collaborative project between NSPO
(National Space Program Office) of Taiwan and UCAR
(University Corporation for Atmospheric Research) of the United States
of America. Initiated in December 1997, the project
will launch a LEO constellation of six microsatellites to collect
atmospheric remote sensing data for operational weather prediction,
climate, ionospheric (space weather monitoring), and geodesy research.
NSPO is the prime sponsor and owner of the
satellites. UCAR, located at NCAR in Boulder, CO, is primarily
sponsored by NSF (National Science Foundation). Other
partners in the project include JPL, NRL, USAF, NOAA, CWB (Central
Weather Bureau of Taiwan), industry from both
countries, universities, and other research organizations from the US,
Taiwan, and other countries. 1) 2)
The overall objective of
ROCSat-3/COSMIC is to extend the low-cost research approach of
refractive GPS radio occultation measurements (to derive important
weather and climate research parameters, including atmospheric
temperature, moisture, and pressure), that began with the GPS/MET
instrument on Microlab-1 (launch April 3, 1995), to the next step by
testing the ability of a constellation of six "ROCSat-3/COSMIC
microsatellites with GPS/MET heritage" to provide the data
needed to fully evaluate the impact of this promising new observational
tool. A goal is also to demonstrate the utility of
atmospheric/ionospheric limb soundings in operational weather
prediction, space weather monitoring and space geodesy. In addition to
carrying an advanced version of the JPL-developed GPS receiver for
occultation measurement, each satellite will
carry two tiny, simple secondary instruments (tri-band-beacon and
photometer) which synergistically enhance the accuracy
and utility of the ionospheric observations. A global data collection
network and operations center will process space and
ground observations and deliver products to users in real-time for
operational impact studies. 3) 4) 5) 6) 7) 8) 9)
Note: A public naming competition took place in Taiwan in 2004 with regard to the ROCSat satellite program. At the end of
this contest, the ROCSat program was given the new name of FormoSat in December 2004. Hence, the ROCSat-3 constellation became FormoSat-3. In USA, FormoSat-3 is known under the name of COSMIC (Constellation Observing System for
Meteorology, Ionosphere and Climate).
Figure 1: Artist's illustration of FormoSat-3/COSMIC spacecraft (image credit: NSPO)
Spacecraft:
Orbital Sciences Corporation (OSC)
of Dulles, VA, USA is the prime contractor for the microsatellites,
selected by NSPO. A
joint team of the OSC and NSPO engineers designed and developed the
satellites, with the early phase of the work performed
at OSC and integration and test performed at NSPO. Several domestic
industry companies of Taiwan were selected to participate in the
project by providing satellite components. The following list gives an
idea of the involvement: 10) 11)
• Satellite computer (Acer Technologies Inc.)
• Mission interface unit (Acer Technologies Inc.)
• Solar sensor (Shihlin Electric & Engineering/eBright Corp.)
• Rechargeable storage battery (Shihlin Electric & Engineering/eBright Corp.)
• Current converter (Shihlin Electric & Engineering/eBright Corp.)
• Satellite antennas (Victory Industrial Corp.)
• Receiving coupler (Victory Industrial Corp.)
• Transmitting filter (Victory Industrial Corp.)
• Satellite heating elements (Yung Tien Industrial Co.)
The S/C structure is of Orbcomm
heritage (MicroStar bus), a cylindrical shape of 1.03 m diameter and
about 18 cm in height
(width). On orbit, two solar panels deploy on each side of the
satellite. All spacecraft are identical, with a mass of about 69 kg
(including fuel). Each S/C features on-board propulsion to reach its
final destination orbit. The ADCS (Attitude Determination and Control
Subsystem) provides attitude knowledge (±5º roll and yaw,
±2º pitch) with an Earth limb sensor and a magnetometer.
Power (46 W) is provided by a solar array and 10 Ah batteries. The
propulsion system consists of two tanks to store
propellant (hydrazine) and 4 small monopropellant thrusters. The design
life is 2 years (5 years expendables). 12) 13)
RF communications: The communication
subsystem consists of an S-band receiver, an L-band transmitter, and a
set of S-band and L-band antennas.
Figure 2: Inside view of the FormoSat-3/COSMIC spacecraft (image credit: NRL, UCAR) 14)
Launch: A launch of the constellation of 6 identical spacecraft took place on April 15, 2006 (UTC) from VAFB, CA. The
low-cost nature of the mission required a special launch and deployment design of the constellation: 15)
• All six spacecraft were
launched in a single shot by a Minotaur vehicle of OSC into one orbital
plane. Minotaur has the
capability to lift the six satellites into an initial circular parking
orbit of about 500 km altitude with an inclination of 72º.
• This is being followed by a
13 month constellation deployment/distribution sequence. Each satellite
will be separated
from the launch vehicle individually. After in-orbit checkout, each
satellite will be boosted by on-board thrusters to different altitudes
ranging up to 800 km. The corresponding different rates of orbit nodal
precession will then gradually drift the
orbit planes apart, until a more-or-less even distribution of six orbit
planes is achieved. The satellites will already start collecting
atmospheric soundings during the orbit-adjustment and constellation
distribution period. 16)
•
The spacecraft deployment occurs in an inverse sequence (6th satellite
first). The total deployment time is estimated to be
387 days. During the transition phase, there are 121 days for the 5th
and 4th satellites in tandem flight, and 198 days for the 3rd
and 2nd satellites in tandem flight. These temporary configurations are
being used for the gravity study to determine the high
order harmonics of the geopotential from the GPS data.
Figure 3: Spacecraft distribution in orbit after a series of initial orbit adjustments (image credit: NSPO)
Orbit of constellation: Circular orbits, altitudes of 800 km, inclinations of 72º; there are 6 operational planes with 1 satellite
per plane, spaced 24º apart.
Ground segment:
The ground segment of FormoSat-3/COSMIC consists of three ground TT&C stations and a MOC (Mission Operations
Center). The three stations are located in Taiwan, Fairbanks (Alaska), and Kiruna (Sweden). The MOC is embedded into
NSPO's MMC (Multi-Mission Center). The MOC performs all S/C operations.
All science and some telemetry data
is being sent to CDAAC (COSMIC Data Analysis and Archive Center) in
Boulder, CO,
and to TACC (Taiwan Analysis Center for COSMIC), a mirror site of CDAAC
in Taiwan, located at CWB (Central Weather
Bureau) in Taipei. The centers also receive data from a global network
of ground GPS and TBB (Tri-Band Beacon Transmitter) receiving sites
(the so-called fiducial network). The centers analyze the received data
and distribute it to the principal
investigators and to the science community for operational evaluation
and research.
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Downlink Parameters
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Uplink Parameters
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Receiver frequency
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1690-1700 MHz (L-band)
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Transmitter frequency
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2025-2120 MHz
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Polarization
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Left Hand Circular
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Polarization
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Left Hand Circular
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Data rates
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Up to 2 Mbit/s
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Data rate
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Up to 32 kbit/s
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Protocol
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CCSDS compatible
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Protocol
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CCSDS compatible
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Table 1: FormoSat-3/COSMIC communication characteristics
During the initial two years of the mission, the science data will be made available through the FormoSat-3/COSMIC project
websites without charge.
POD (Precise Orbit Determination) of the constellation is required for data analysis.
Mission status: The FormoSat-3 constellation is operating nominally as of 2007. All satellites are in good health and providing initial data. 17) 18)
• As of Aug. 2007, the
satellite constellation is approaching final deployment with only one
more spacecraft, FM1, remaining its initial 500 km orbit (Figure 4). Presently the system is producing 1500-1700 good neutral atmospheric soundings per
day with an average latency of about 2 hours. 19)
• Maneuvers continue to move the satellites into their final orbits. As of Jan. 2007, FM2 and FM5 are at 800 km altitude
while FM6 is at 716 km. FM1, FM3 and FM4 are still at 518 km.
• The satellites are averaging about 1,200 soundings a day, in a nearly uniform global distribution, providing independent
data over vast stretches of ocean and ice where there are no weather balloons. As the satellites approach their final positions,
they will increase their output to about 2,500 soundings a day. 20)
• The first set of occultation data from FormoSat-3 was obtained on April 21, 2006.
• Cosmic data became available to the public on July 28, 2006. JPL and its partners have begun processing Cosmic data into
temperature and water vapor profiles of the atmosphere and measurements of the electron content of the ionosphere.
Figure 4: The deployment timeline of the FormoSat-3/COSMIC constellation (image credit: NSPO)
Sensor complement: (IGOR, TIP, CERTO/TBB)
The FormoSat-3/COSMIC constellation
produces about 3000 soundings (minimum requirement of 2500/day) of
bending
angle and refractivity globally in all weather each day for at least
one year after the spacecraft are placed in their final orbits.
From these soundings, estimates of electron density in the ionosphere
and temperature, water vapor and pressure in the
stratosphere and troposphere will be derived. Desirable characteristics
of these data include such items as: high accuracy, high
vertical resolution, all weather (clouds and aerosols do not affect
measurements), no calibration of instrument required, no
instrument drift, require no first guess, modest cost.
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Parameter
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Science requirement
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Comment
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Vertical GPS occultation resolution
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0.3-1.5 km
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0.3 km near surface, 1.5 km at 45 km
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Horizontal GPS occultation resolution
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300-600 km
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Smaller for fronts with large slope
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Bending angle profile
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1.5 x 10-6 rad
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Limited mainly by residual ionospheric error and data noise
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Refractivity profile
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<1%
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As good as 0.2% between 10-30 km
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Temperature profile
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1º C
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In 0-40 km height range, assuming dry air
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Water vapor profile
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<1-10%
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Between 0-5 km, assuming model temp. error of 1-2º, errors
between 5-10 km are larger
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Geopotential height vs pressure
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10-20 m
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Between 0-30 km (worse at solar maximum)
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Electron density profile
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<1-20%
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Profile quality near the F2 peak, can be worse elsewhere;
limited by horizontal gradients
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GPS TEC (Total Electron Content)
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0.001 TECU (Total Electron
Content Unit)
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Relative TEC (absolute about 3-5 TECU)
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TBB TEC
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0.003 TECU
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Relative TEC (absolute about 1-3 TECU)
|
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TIP peak for F2 density, NmF2
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<1-10%
|
Performs better at high electron densities
Works only on the night side of the globe
|
|
Magnetometer measurement
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10 nT
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Precision at 1 Hz rate, 500 NT accuracy
|
|
Scintillation GPS
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N/A
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100 Hz SNR data used to determine S4
|
|
Scintillation TBB
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N/A
|
50-1000 Hz SNR data
|
|
LEO position knowledge
|
about 10 cm
|
3-D rms position error (not critical)
|
|
LEO velocity knowledge
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<0.1 mm/s
|
Relative velocity error for paired satellites
|
|
|
|
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Table 2: Science requirements of the FormoSat-3/COSMIC constellation
|
Number of occultation measurements
|
About 2500 soundings/day on a global scale
|
|
L1/L2 phase measurements
|
About 2 mm (10 s interval for precise orbit determination)
|
|
GPS phase sampling rate
|
0.1-50 Hz
|
|
GPS vertical range neutral atmosphere
|
Surface to 60 km (50 Hz sampling)
|
|
GPS vertical range ionosphere
|
90-800 km (10 Hz sampling)
|
|
TBB phase measurement
|
<32 mm at 150 MHz (ground receiver)
|
|
TBB sampling rate
|
>50 Hz (ground receiver)
|
|
TIP measurement
|
<10% (uncertainty in photon count)
|
|
TIP footprint
|
125 km x 25 km (at 400 km height of F2 layer)
|
|
TIP resolution
|
0.1-10 s averaging
|
|
Magnetometer
|
10 nT precision, 500 nT accuracy
|
Table 3: Observational requirements of FormoSat-3/COSMIC
IGOR (Integrated GPS Occultation Receiver), based on the BlackJack GPS
occultation receiver design of JPL and flown on
such missions as CHAMP, SAC-C, and GRACE. IGOR, built by Broad Reach
Engineering of Tempe, AZ, is the primary
science instrument of the FormoSat-3/COSMIC constellation. The IGOR
receivers, on FormoSat-3/COSMIC will be able
to track all GPS satellites in view simultaneously, including two or
more occulting satellites. It will operate fully autonomously,
scheduling when to track which satellites and at what sampling rate
based on its own known position and those of the GPS
satellites. The instrument reports high-rate (50 Hz) dual frequency
carrier phase measurements on the occulting links with
sub-millimeter precision for accurate, high resolution profiling. Lower
rate (0.1 Hz) phase measurements of all satellites in
view are being collected for precise orbit determination (POD) at the
5-10 cm level.
IGOR tracks both GPS carrier
frequencies (L1, L2) to separate the frequency-dependent (dispersive)
ionospheric delay
from the non-dispersive refractive delay of the neutral atmosphere. A
patented "semi-codeless" technique is used to obtain
precise measurements of the L2 signal, both carrier phase and
pseudorange, with anti-spoofing turned on. In addition to
these measurements, the GPS instrument can record GPS signal amplitudes
for on-orbit ionospheric scintillation monitoring
and correction of signal diffraction effects in post-processing. The
instrument mass is 4.6 kg; size of about 20 cm x 24 cm x 10.5
cm; power of 16 W nominal, 23 W peak, antenna inputs: 4. 21) 22)
Figure 5: Illustration of the IGOR instrument (image credit: Broad Reach Engineering)
The GPS radio occultation technique
is based on the following principles: As a signal travels through the
atmosphere it is
retarded and bent. This results in a phase and Doppler shift, which can
be measured very accurately by the GPS receiver
aboard the LEO FormoSat-3/COSMIC satellites. Since the transmitter and
receiver positions and velocities are accurately
know from precise orbit determination, the signal bending angle alpha
as a function of impact parameter, can be computed
from the Doppler shift observed at LEO. From the basic bending angle
versus impact parameter data, vertical profiles of refractivity as a
function of tangent point radius can be derived. Further analysis
converts refractivity to electron density in the
ionosphere.
Figure 6: Occultation scheme of GPS signals with LEO satellites (image credit: Broad Reach Engineering)
TIP (Tiny Ionosphere Photometer) a nadir-viewing instrument, designed and built by NRL (Naval Research Laboratory),
Washington, DC and Praxis Inc. TIP and TBB provide measurements of electron density, an important parameter of the upper
atmosphere. The readings of TIP and TBB complement the primary IGOR instrument so that 3-D fields of electron density
gradients between 90 and 750 km can be inferred.
TIP is a compact, narrow-band, ultraviolet photometer operating at the 135.6 nm wavelength (UV radiation). This emission
is produced by recombination of O+
ions and electrons, which is the natural decay process for the
ionosphere. At night, the
strength of the emission is proportional to the product of the square
of the peak electron density; during the daytime the emission is
dominated by photoelectron impact excitation of atomic oxygen and is
not useful for ionospheric sensing. 23) 24) 25) 26)
Figure 7: TIP electronics module (top) and sensor module (image credit: NRL)
In particular TIP provides
horizontal gradients in ionospheric electron density at the peak of the
F2 layer, along the satellite
orbit track. TIP measures the naturally occurring nighttime emission of
neutral oxygen at 135.6 nm. This emission (airglow) is
produced by the recombination of O + ions and electrons and is
proportional to the square of the electron density in the ionospheric F
region. Since horizontal gradients of electron density are a limiting
error source for occultation inversions in the
ionosphere, the combined analysis of TIP and GPS data promises improved
retrievals of nighttime ionospheric profiles.
TIP is nadir-pointing with a
3.8º circular FOV providing a 30 km horizontal resolution from an
orbital altitude of 800 km. The
TIP sensor module consists of:
• Photomultiplier tube observing UV light
• Strontium fluoride filter passes 131-160 nm emissions
• Very high sensitivity ~150 counts/s/Rayleigh
Figure 8: Illustration of the TIP filter wheel (image credit: NRL)
CERTO/TBB (Coherent
Electromagnetic Radio Tomography/Triband Beacon Transmitter), designed
and built at NRL.
CERTO/TBB transmits phase data measurements at 150, 400 and 1067 MHz
(VHF, UHF, L-band) which can be received at
ground stations worldwide. These data are converted to line-of-sight
TEC (Total Electron Content) observations that can
be processed with 2-dimensional ionospheric tomography techniques.
CERTO/TBB data can also be combined with the other ionospheric
observations in tomographic and physical data assimilation models to
compute global four-dimensional electron density fields. 27) 28) 29) 30) 31)
The FormoSat-3/COSMIC instrument
suite permits three-dimensional tomography of the ionosphere with
unprecedented
resolution and accuracy. FormoSat-3/COSMIC data will be highly
complementary to other satellite sounding systems, including
radiometric sounders on the POES and GOES series satellites of NOAA.
The independence and the high-vertical
resolution of the radio occultation soundings complement the high
horizontal resolution of the radiometric soundings and
together the two systems can likely be combined to yield composite
soundings of temperature and water vapor with unprecedented accuracy,
horizontal and vertical resolution, and global coverage.
Figure 9: Photo of the CERTO instrument (image credit: NRL)
Figure 10: CERTO/TBB accommodation on FormoSat-3/COSMIC (image credit: NRL)
Figure 11: Joint CERTO/TBB, GPS-GOX, TIP operations on FormoSat-3/COSMIC (image credit: NRL)
1)
L.C. Lee, C. Rocken, "Applications of Constellation Observing System
for Meteorology, Ionosphere & Climate", R. Kursinski (Ed.),
Springer, 2000, ISBN
962-430-135-2
2)
C. Rocken, Y. H. Kuo, W. S. Schreiner, D. Hunt, S. Sokolovskiy, C.
McCormick, "COSMIC System Description," Special issue of TAO
(Terrestrial, Atmospheric
and Oceanic Science), Vol. 11, No. 1, March 2000, pp.21-52
3)
G. A. Hajj, L. C. Lee, X. Pi, L. J. Romans, et al., COSMIC GPS
Ionospheric Sensing and Space Weather," Special issue of TAO
(Terrestrial, Atmospheric and
Oceanic Science), Vol. 11, No. 1, March 2000, pp.235-272
4)
Y. K. Kuo, L. C. Lee, "A Constellation of Microsatellites Promises to
Help in a Range of Geoscience Research," EOS Transcriptions, AGU, Vol.
80, No. 40, Oct.
5, 1999, pp. 467-471
5) http://www.cosmic.ucar.edu/
6) Information provided by Paul Chen of NSPO
7)
E. B. Pavlis, C. Chao, C. Hwang, C. Liu, C. Shum, C. Tseng, M. Yang,
"Geodetic applications of the ROCSat-3/COSMIC mission, Towards an
Integrated Global
Geodetic Observing System (IGGOS)," International Association of
Geodesy Symposia, Vol. 120, editors: R. Rummel, H. Drewes, W. Bosch, H.
Hornik, pp.
214-217, Springer-Verlag Berlin, Germany, October, 1998
8) http://www.nspo.org.tw/2005e/projects/project3/intro.htm
9) Y. H. Kuo, C. Rocken, R. A. Anthes, "Constellation Observing System for Meteorology, Ionosphere and Climate (COMIC)," URL:
http://ams.confex.com/ams/pdfpapers/82660.pdf
10) http://www.nspo.org.tw/2005e/projects/project3/component.htm
11) http://www.ucar.edu/news/releases/2006/cosmicfacts.shtml
12) http://www.orbital.com/SatellitesSpace/LEO/FORMOSAT-3/index.html
13) FormoSat-3/COSMIC, http://www.orbital.com/NewsInfo/Publications/FORMOSAT-3_Fact.pdf
14)
P. A. Bernhardt, C. L. Siefring. A. Yau,"Space Based Systems for
Ionospheric Density and Scintillation Mapping in Conjunction with
Incoherent Scatter Radars,"
AMISR Science Planning Meeting, Asilomar, CA, Oct. 12, 2006 URL:
http://www.amisr.com/meetings/2006asilomar/presentations/Bernhardt/AMISRSpaceBasedPoster.ppt
15)
A. M. Wu, C. J. Shieh, V. Chu, "ROCSat-3 Constellation Design and Data
Simulation," Proceedings of 53rd IAC and World Space Congress, 2002,
Oct. 10-19,
2002, Houston, TX, IAF-02-A.7.06
16)
Note: Earth oblateness is the reason for the orbital plane drifts. The
nodal precession, a well-known gravity phenomenon, is for instance
being used by all spacecraft
in sun-synchronous orbit to compensate for the Earth's revolution
around the sun (about 0.9856º per day).
17)
C.-H. Vicky Chu, S.-K. Yang, C.-J. Fong, N. Yen, T.-Y. Liu, W.-J. Chen,
D. Hawes, Y.-A. Liou, B. Kuo, "The Most Accurate and Stable Space-Borne
Thermometers - FORMOSAT-3/COSMIC Constellation," Proceedings of the
21st Annual AIAA/USU Conference on Small Satellites, Logan, UT, USA, Aug.
13-16, 2007, SSC07-VII-1
18) Annual AMS (American Meteorological Society) Meeting 2007, San Antonio, TX, USA, Jan. 15-18, 2007, N. Yen, URL:
http://www.cosmic.ucar.edu/AMS2007/AMS_NICK_011507.ppt
19) Latest Status update - Aug. 23, 2007, URL: http://www.cosmic.ucar.edu/
20)
An-Ming Wu, Lance Wu, "Integrated Mission Planning for FormoSat-2
Imaging Satellite and FormoSat-3 Meteorological Constellation,"
Proceedings of the
57th IAC/IAF/IAA (International Astronautical Congress), Valencia,
Spain, Oct. 2-6, 2006, IAC-06-B1.6.09
21) http://www.broad-reach.net/igor06.html
22) http://www.cosmic.ucar.edu/systems/IGOR_Flyer.pdf
23)
C. Coker, K. F. Dymond, S. A. Budzien, D. Chua, "First Observations of
the Ionosphere Using the Tiny Ionospheric Photometer," Taipei, Taiwan,
FormoSat-3/COSMIC Workshop 2006 - Early Results and IOP Campaigns, Nov.
28-Dec. 1, 2006, URL:
http://www.cosmic.ucar.edu/oct2006workshop/presentations/Coker_Clayton_20061017.ppt
24)
P. C. Kalmanson, S. A. Budzien, C. Coker, K. F. Dymond, "The tiny
ionospheric photometer instrument design and operation," Proceedings of
SPIE, `Instruments,
Science, and Methods for Geospace and Planetary Remote Sensing,' Carl
A. Nardell, Paul G. Lucey, Jeng-Hwa Yee, James B. Garvin, editors, Vol.
5660,
Bellingham, WA, Dec. 2004, pp. 259-270
25)
C. Coker, K. F. Dymond, S. A. Budzien, "Using the Tiny Ionospheric
Photometer (TIP) on the COSMIC Satellites to Characterize the
Ionosphere," American
Geophysical Union (AGU) Fall Meeting San Francisco, CA, Dec. 6-10, 2002
26)
K. F. Dymond, J. B. Nee, R. J. Thomas, 2000: "The Tiny Ionospheric
Photometer: An Instrument for Measuring Ionospheric Gradients for the
COSMIC
Constellation," Terrestrial, Atmospheric and Oceanic Sciences, Vol. 11,
2000, pp. 273-290.
27)
P. A. Bernhardt, C. E. Coker, "New TEC Data Sources from Radio Beacon
Monitors of the Ionosphere," LWS Geostorm CDAW and Conference Florida
Tech,
Melbourne, FL, March 8, 2007, URL: http://www.cosmic.ucar.edu/aug2002workshop/presentations/rocken_pres.ppt
28)
P. A. Bernhardt, C. A. Selcher, S. Basu, G. Bust, S. C. Reising, 2000:
"Atmospheric studies with the Tri-Band Beacon instrument on the COSMIC
constellation,"
Terrestrial, Atmospheric and Oceanic Sciences, Vol. 11, No 1, March
2000, pp. 291-312
29)
P. A. Bernhardt, C. L. Siefring, "The CERTO and CITRIS Instruments for
Radio Scintillation and Electron Density Tomography from the C/NOFS,
COSMIC,
NPSAT1 and STPSAT1 Satellites," The 2004 Joint Assembly (of CGU, AGU,
SEG and EEGS), Montreal, Canada, May 17.21, 2004
30)
P. A. Bernhardt, C. L. Siefring, T. W. Garner, T. L. Gaussiran, J.
Secan, F. Smith, K. Groves, "First Results for the TBB/CERTO Beacon
Experiment on FormoSat-
3/COSMIC," AGU (American Geophysical Union) Fall Meeting, 2006, San,
Francisco, CA, USA, Dec. 11-15, 2006
31) P. A.
Bernhardt, C. L. Siefring, J. D. Huba, C. A. Selcher, CITRIS: The
Cosmic Companion for LEO Radio Occultation," COSMIC Radio Occultation
Workshop,
Aug. 21, 2002, Boulder, CO, USA, URL: http://www.cosmic.ucar.edu/aug2002workshop/presentations/
This description was provided by Herbert J. Kramer from his documentation of: "Observation of the Earth and Its Environment: Survey of Missions and Sensors" - comments and corrections to this article are welcomed by the author.
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